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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Earth Sci.</journal-id>
<journal-title>Frontiers in Earth Science</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Earth Sci.</abbrev-journal-title>
<issn pub-type="epub">2296-6463</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">876196</article-id>
<article-id pub-id-type="doi">10.3389/feart.2022.876196</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Earth Science</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Particle Size and Internal Structure of Deformed Coal: Microstructure and Adsorption/Desorption Characteristics of CO<sub>2</sub> and CH<sub>4</sub>
</article-title>
<alt-title alt-title-type="left-running-head">Li et al.</alt-title>
<alt-title alt-title-type="right-running-head">Particle Size and Internal Structure of Deformed Coal</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Li</surname>
<given-names>Xiaoshi</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1566634/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Ju</surname>
<given-names>Yiwen</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1310688/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Song</surname>
<given-names>Yu</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Yan</surname>
<given-names>Zhifeng</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff5">
<sup>5</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Li</surname>
<given-names>Qiangguang</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff6">
<sup>6</sup>
</xref>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>Key Laboratory of Computational Geodynamics</institution>, <institution>College of Earth and Planetary Sciences</institution>, <institution>University of Chinese Academy of Sciences</institution>, <addr-line>Beijing</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Institute of Geomechanics</institution>, <institution>Chinese Academy of Geological Sciences</institution>, <addr-line>Beijing</addr-line>, <country>China</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>Key Laboratory of Paleomagnetism and Tectonic Reconstruction</institution>, <institution>Ministry of Natural Resources</institution>, <addr-line>Beijing</addr-line>, <country>China</country>
</aff>
<aff id="aff4">
<sup>4</sup>
<institution>Key Laboratory of Coalbed Methane Resource &#x26; Reservoir Formation Process</institution>, <institution>Ministry of Education</institution>, <institution>School of Resources &#x26; Earth Science China University of Mining and Technology</institution>, <addr-line>Xuzhou</addr-line>, <country>China</country>
</aff>
<aff id="aff5">
<sup>5</sup>
<institution>School of Earth Science and Engineering</institution>, <institution>Hebei University of Engineering</institution>, <addr-line>Handan</addr-line>, <country>China</country>
</aff>
<aff id="aff6">
<sup>6</sup>
<institution>Key Laboratory of Karst Georesources and Environment</institution>, <institution>Ministry of Education</institution>, <institution>College of Resource and Environmental Engineering</institution>, <institution>Guizhou University</institution>, <addr-line>Guiyang</addr-line>, <country>China</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1368166/overview">Candan Gokceoglu</ext-link>, Hacettepe University, Turkey</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1706303/overview">Hasril Hasini</ext-link>, Universiti Tenaga Nasional, Malaysia</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1447721/overview">Hongjian Zhu</ext-link>, Yanshan University, China</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Yiwen Ju, <email>juyw03@163.com</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Economic Geology, a section of the journal Frontiers in Earth Science</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>04</day>
<month>05</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>10</volume>
<elocation-id>876196</elocation-id>
<history>
<date date-type="received">
<day>15</day>
<month>02</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>19</day>
<month>04</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Li, Ju, Song, Yan and Li.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Li, Ju, Song, Yan and Li</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>Structural deformation has a very important effect on the particle size and adsorption/desorption properties of coal, which is widely distributed in China, but there are few studies in this area. The effects of particle size and internal structure on the pores and adsorption properties of deformed coal were studied, and the influence of structural deformation was analyzed. Eight undeformed and deformed coal samples were progressively crushed from 0.12 to 0.15&#xa0;mm (100&#x2013;120 mesh), 0.18&#x2013;0.25&#xa0;mm (60&#x2013;80 mesh), and 0.42&#x2013;0.84&#xa0;mm (20&#x2013;40 mesh), and subsequently, adsorption/desorption characteristics of CO<sub>2</sub> and CH<sub>4</sub> and pore structure analyses were performed on all the grain size fractions. The coal size fraction has a slightly smaller influence on CO<sub>2</sub> adsorption than on CH<sub>4</sub> adsorption. Deformation can promote gas desorption, which increases as the deformation increases. Moreover, deformation can reduce the effect of granularity and internal structure on gas adsorption capacities. The 60&#x2013;80 mesh is suggested to be the optimal size for deformed coal to achieve the ideal adsorption/desorption effect without eliminating the influence of structural deformation. However, below 100&#x2013;120 mesh is recommended to reduce the impact of structural deformation on data processing and analysis when the sample contains both deformed and undeformed coals.</p>
</abstract>
<kwd-group>
<kwd>deformed coal</kwd>
<kwd>particle size</kwd>
<kwd>internal structure</kwd>
<kwd>microstructure</kwd>
<kwd>adsorption/desorption characteristics</kwd>
</kwd-group>
<contract-num rid="cn001">41672201 41530315 40972131 41202120</contract-num>
<contract-sponsor id="cn001">National Natural Science Foundation of China<named-content content-type="fundref-id">10.13039/501100001809</named-content>
</contract-sponsor>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>Coal is a complex polymeric material with a complex pore structure. Most scholars consider that coalbed methane (CBM) in coal seams mainly exists in an adsorbed state (<xref ref-type="bibr" rid="B3">Cao and Zhang, 2003a</xref>, <xref ref-type="bibr" rid="B5">Cao et al., 2003b</xref>; <xref ref-type="bibr" rid="B1">Busch et al., 2003</xref>; <xref ref-type="bibr" rid="B26">Ju and Li, 2009</xref>). Therefore, the coal adsorption property is an important index of the release of coal seam gas. Studies on coal adsorb ability have been extremely significant in the development of CBM and for predictions of the gas content (<xref ref-type="bibr" rid="B15">Gayer and Harris, 1996</xref>; <xref ref-type="bibr" rid="B9">Cui et al., 2005</xref>; <xref ref-type="bibr" rid="B19">Islam and Hayashi, 2008</xref>). The main factors that are currently considered to affect coal adsorption are the composition, mineral content, temperature, pressure, metamorphic degree, and structural deformation (<xref ref-type="bibr" rid="B8">Crosdale and Beamish, 1993</xref>; <xref ref-type="bibr" rid="B1">Busch et al., 2003</xref>; <xref ref-type="bibr" rid="B44">Qu, 2011</xref>; <xref ref-type="bibr" rid="B61">Zou and Rezaee, 2016</xref>; <xref ref-type="bibr" rid="B13">Li et al., 2019a</xref>; <xref ref-type="bibr" rid="B35">Li et al., 2019b</xref>). Many scholars have reported that the coal adsorption capacity increases with the metamorphic degree for <italic>R</italic>
<sub>o, max</sub> &#x3c; 4.0% (<xref ref-type="bibr" rid="B54">Yao and Liu, 2007</xref>; <xref ref-type="bibr" rid="B23">Jiang et al., 2010</xref>). Zhong et al. found that the coal adsorption capacity for methane decreased as the temperature increased, and this change was more marked at higher pressures (<xref ref-type="bibr" rid="B57">Zhong et al., 2002</xref>). Hou et al. characterized the pore structure of coals with different particle sizes that formed under structural deformation and reported that structural deformation increases the abundance of accessible mesopores and causes micropore collapse <xref ref-type="bibr" rid="B20">Hou et al. (2017)</xref>. Pan et al. studied the effects of temperature and pressure on the adsorption capacity of deformed coal, which was found to decrease as the temperature increased and was significantly higher for ductile deformed coal than for weak brittle deformed coal <xref ref-type="bibr" rid="B41">Pan et al. (2012)</xref>. Qu et al. found that the adsorption capacity of deformed coal increased significantly with deformation because of the deformation-induced formation of a complex pore system <xref ref-type="bibr" rid="B44">Qu, (2011)</xref>; (<xref ref-type="bibr" rid="B60">Zhu et al., 2018</xref>, <xref ref-type="bibr" rid="B59">2020</xref>).</p>
<p>Many studies have been conducted on the effect of sample size on the adsorption/desorption properties of coal (<xref ref-type="bibr" rid="B56">Zhang et al., 2009</xref>; <xref ref-type="bibr" rid="B47">Sun et al., 2012</xref>; <xref ref-type="bibr" rid="B18">Han et al., 2013</xref>; <xref ref-type="bibr" rid="B21">Jia et al., 2013</xref>; <xref ref-type="bibr" rid="B62">Marcin et al., 2016</xref>; <xref ref-type="bibr" rid="B37">Mastalerz et al., 2017</xref>). For example, through CH<sub>4</sub> adsorption experiments with different particle sizes, Sun et al. reported that the smaller the particle size is, the larger the specific surface area and adsorption capacity (<xref ref-type="bibr" rid="B56">Zhang et al., 2009</xref>); <xref ref-type="bibr" rid="B47">Sun et al. (2012)</xref>. Jia et al. conducted CH<sub>4</sub> adsorption/desorption experiments on coal with different particle sizes (0.2&#x2013;0-0.5&#xa0;mm, 0.5&#x2013;1-1 and 1.3&#xa0;mm) and believed that within a certain time range, the particle size of coal is inversely proportional to the total gas desorption <xref ref-type="bibr" rid="B21">Jia et al. (2013)</xref>. However, one of the most common problems associated with adsorption/desorption property studies on coal samples is the particle size of samples chosen for the experiments. In the vast majority of laboratory sorption experiments, the samples are crushed and sieved to a given fraction before the experiment starts, which influences the experimental data and analysis. Regarding coals, the fraction that passed through a 60 mesh (0.25&#x2013;0.2&#xa0;mm) sieve has been preferred, but other analytical size fractions have also been used, including but not limited to 4 mesh (&#x3c;4.78&#xa0;mm), 7 mesh (&#x3c;2.83&#xa0;mm) (<xref ref-type="bibr" rid="B14">Furmann et al., 2016</xref>), 16 mesh (&#x3c;1.18&#xa0;mm) (<xref ref-type="bibr" rid="B48">Swanson et al., 2015</xref>), 100 mesh (&#x3c;0.125&#xa0;mm) and 200 mesh (&#x3c;0.074&#xa0;mm) (<xref ref-type="bibr" rid="B4">Cao et al., 2015</xref>; <xref ref-type="bibr" rid="B50">Wang and Ju, 2015</xref>; Marcin et al., 2016). Mastalerz et al. studied N<sub>2</sub> and CO<sub>2</sub> adsorption in coal and shale for different particle sizes [chunks (&#x223c;7&#xa0;mm) to 4 mesh (&#x3c;4.78&#xa0;mm), 7 mesh (&#x3c;2.83&#xa0;mm), 18 mesh (&#x3c;1&#xa0;mm), 30 mesh (0.595&#xa0;mm), 60 mesh (&#x3c;0.250&#xa0;mm), 200 mesh (&#x3c;0.074&#xa0;mm), and 230 mesh (&#x3c;0.063&#xa0;mm)] and determined that the most suitable particle sizes for adsorption analysis were the 60-mesh fraction for coal and 200 mesh fractions for shales (<xref ref-type="bibr" rid="B37">Mastalerz et al., 2017</xref>).</p>
<p>Complex tectonic movement has produced widely developed deformed coals in most coal-bearing basins in China (<xref ref-type="bibr" rid="B3">Cao and Zhang, 2003a</xref>, <xref ref-type="bibr" rid="B5">Cao et al., 2003b</xref>; <xref ref-type="bibr" rid="B24">Ju et al., 2005a</xref>). Deformation crushes coal and affects its pore structure and macromolecular structure, which in turn affects adsorption and desorption in this material (<xref ref-type="bibr" rid="B10">Domazetis and Raoarun, 2008</xref>; <xref ref-type="bibr" rid="B7">Chen et al., 2011</xref>; <xref ref-type="bibr" rid="B38">Mathews et al., 2011</xref>; <xref ref-type="bibr" rid="B6">Castro and Lobodin, 2012</xref>; <xref ref-type="bibr" rid="B2">Cai et al., 2013</xref>; <xref ref-type="bibr" rid="B31">Li et al., 2014</xref>). However, relatively few studies have been performed on the adsorption performance of deformed coal of different particle sizes. When the adsorption performance and pore structure of deformed coal are studied, the selection of sample size fractions will affect the results. If the coal samples collected contain deformed coal and undeformed coal, then the sample size should be selected to be the most appropriate during the experiment because the influence of structural deformation on the particle size and pore structure of coal cannot be ignored. Therefore, in this paper, we collected samples of brittle and ductile deformed coal to perform a comparative analysis using undeformed coal as a reference. We conducted experiments on the isothermal adsorption of CH<sub>4</sub> and CO<sub>2</sub> in coal of different particle sizes to investigate the effect of deformation and particle size and internal structure on the coal adsorption performance. The suitable experimental size range of deformed coal is also discussed.</p>
</sec>
<sec id="s2">
<title>2 Samples and Methods</title>
<sec id="s2-1">
<title>2.1 Geological Settings and Samples</title>
<p>All coal samples were collected from the Permo-Carboniferous coalbed in the Huainan-Huaibei coalfield, which was strongly affected by Mesozoic tectonic deformation (<xref ref-type="fig" rid="F1">Figure 1</xref>). The coal seams are distributed mainly in the graben part, especially in the syncline part. A series of multiple synclines and anticlines are distributed in this area with a NNW-NE strike. The structural deformation remarkably destroyed the structure of coal seams, resulting in the widespread development of brittle and ductile deformed coal in this area (<xref ref-type="bibr" rid="B24">Ju et al., 2005a</xref>; <xref ref-type="bibr" rid="B34">Li et al., 2012</xref>).</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>The samples distribution plot (after <xref ref-type="bibr" rid="B24">Ju et al., 2005a</xref>; <xref ref-type="bibr" rid="B34">Li et al., 2012</xref>).</p>
</caption>
<graphic xlink:href="feart-10-876196-g001.tif"/>
</fig>
<p>Deformed coal is formed under one or more periods of tectonic stress. The original structure is deformed (crushed, folded, etc.) or undergoes superimposed damage in different degrees of stress, and even the internal chemical composition and structure are changed (<xref ref-type="bibr" rid="B28">Ju et al., 2004</xref>). Deformed coal can be divided into three types, namely, brittle deformation, ductile deformation and brittle-ductile transition, according to the structural composition and mechanical properties (<xref ref-type="bibr" rid="B63">Hou et al., 1995</xref>; <xref ref-type="bibr" rid="B17">Guo, 2001</xref>; <xref ref-type="bibr" rid="B22">Jiang and Ju, 2004</xref>; <xref ref-type="bibr" rid="B28">Ju et al., 2004</xref>, <xref ref-type="bibr" rid="B24">2005a</xref>, 2009). The brittle deformation series shows the development of one or more groups of joints or fractures. Strong brittle deformation leads to dislocation of the coal particles cut by joints and cracks and is even rounded to form a clastic structure. A ductile deformation series is formed under certain strata temperature and pressure conditions, and the coal seam is ductile deformed under extrusion or shear stress, forming various ductile structures such as folds and flowing deformation (<xref ref-type="bibr" rid="B5">Cao et al., 2003b</xref>; <xref ref-type="bibr" rid="B22">Jiang and Ju, 2004</xref>; <xref ref-type="bibr" rid="B28">Ju et al., 2004</xref>, <xref ref-type="bibr" rid="B24">2005a</xref>, 2009; <xref ref-type="bibr" rid="B49">Wang et al., 2009</xref>; <xref ref-type="bibr" rid="B43">Qu et al., 2012</xref>). Brittle-ductile deformation is a transition type between brittle deformation and ductile deformation.</p>
<p>Eight coal samples in this paper were evaluated according to the above classification. Six deformed coal samples were collected from the Xinzhuangzi, Linhuan and Haizi coal mines. Additionally, to serve as a reference for the deformed coals, we obtained two undeformed coal samples from the Zhangbei coal mine that were almost unaffected by structural deformation (<xref ref-type="fig" rid="F1">Figure 1</xref>). The characteristics of coal hand specimens with different deformation degrees are quite obvious and are described in detail in <xref ref-type="table" rid="T1">Table 1</xref>. All the samples were labeled by the coal type: the undeformed coal samples were labeled P01 and P02; the brittle deformed coal samples were labeled B01, B02, and B03; and the ductile deformed coal samples were labeled D01, D02, and D03 (<xref ref-type="table" rid="T1">Table 1</xref>).</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Coal sample characteristics.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th colspan="2" align="left">Deformation series</th>
<th align="center">Sample No</th>
<th align="center">Deformation degree</th>
<th align="center">Characteristics of macroscopic hand-formed specimens</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td rowspan="2" align="left">Undeformed coal</td>
<td align="left"/>
<td align="left">P01</td>
<td align="left">/</td>
<td rowspan="2" align="left">The undeformed can be observed. The coal is hard and difficult to separate by hand</td>
</tr>
<tr>
<td align="left"/>
<td align="left">P02</td>
<td align="left">/</td>
</tr>
<tr>
<td rowspan="6" align="left">Deformed coal</td>
<td rowspan="3" align="left">Brittle deformation</td>
<td align="left">B01</td>
<td align="left">Weak</td>
<td rowspan="2" align="left">Brittle deformed coal usually has multidirectional or unidirectional fractures, and the undeformed can be observed. The coal is hard and not easily broken</td>
</tr>
<tr>
<td align="left">B02</td>
<td align="left">Weak</td>
</tr>
<tr>
<td align="left">B03</td>
<td align="left">Strong</td>
<td align="left">The undeformed is damaged, and the coalbedding has almost disappeared. The coal has subangular or subround particles and develops small fractures in different directions. The coal has a low strength and can be powderized by hand</td>
</tr>
<tr>
<td rowspan="3" align="left">Ductile deformation</td>
<td align="left">D0s1</td>
<td align="left">Weak</td>
<td rowspan="2" align="left">Wrinkle and mylonitic structure can be observed in the coal. The coal petrographic composition is not easily discriminated. The coal is soft and can be easily pinched into fragments</td>
</tr>
<tr>
<td align="left">D02</td>
<td align="left">Weak</td>
</tr>
<tr>
<td align="left">D03</td>
<td align="left">Strong</td>
<td align="left">The coal petrographic composition is strongly wrinkled and forms irregular crumb structures that cannot be discriminated. The coal can be turned into fine grains or powder by hand</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s2-2">
<title>2.2 Experimental Methods</title>
<p>The metamorphic grade, proximate analysis and component composition after purification of all coal samples were analyzed before the experiment (<xref ref-type="table" rid="T2">Table 2</xref>). The table shows that the coal samples are mainly of low or medium ash, with an ash yield between 8.93 and 44.31%, volatile matter (<italic>V</italic>) content ranging from 10.04 to 34.99%, moisture content varying from 0.79 to 1.84%, and fixed carbon content ranging from 36.35 to 79.05%.</p>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Properties of coal samples.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th rowspan="2" align="left">Sample No</th>
<th rowspan="2" align="center">
<italic>R</italic>
<sub>o, max</sub> (%)</th>
<th colspan="4" align="center">Proximate analysis (air-dried basis, wt%)</th>
<th colspan="4" align="center">Maceral analysis after purification (%)</th>
</tr>
<tr>
<th align="center">
<italic>M</italic>
</th>
<th align="center">
<italic>A</italic>
</th>
<th align="center">
<italic>V</italic>
</th>
<th align="center">
<italic>FC</italic>
</th>
<th align="center">Vitrinite</th>
<th align="center">Inertinite</th>
<th align="center">Liptinite</th>
<th align="center">Mineral</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">P01</td>
<td align="char" char=".">0.97</td>
<td align="char" char=".">1.70</td>
<td align="char" char=".">13.82</td>
<td align="char" char=".">34.99</td>
<td align="char" char=".">49.50</td>
<td align="char" char=".">81.90</td>
<td align="char" char=".">10.09</td>
<td align="center">5.43</td>
<td align="char" char=".">2.57</td>
</tr>
<tr>
<td align="left">P02</td>
<td align="char" char=".">1.29</td>
<td align="char" char=".">0.93</td>
<td align="char" char=".">44.31</td>
<td align="char" char=".">18.42</td>
<td align="char" char=".">36.35</td>
<td align="char" char=".">90.24</td>
<td align="char" char=".">8.79</td>
<td align="center">/</td>
<td align="char" char=".">0.97</td>
</tr>
<tr>
<td align="left">B01</td>
<td align="char" char=".">1.08</td>
<td align="char" char=".">1.33</td>
<td align="char" char=".">8.93</td>
<td align="char" char=".">28.29</td>
<td align="char" char=".">61.45</td>
<td align="char" char=".">95.29</td>
<td align="char" char=".">2.52</td>
<td align="center">/</td>
<td align="char" char=".">2.19</td>
</tr>
<tr>
<td align="left">B02</td>
<td align="char" char=".">1.11</td>
<td align="char" char=".">1.84</td>
<td align="char" char=".">10.41</td>
<td align="char" char=".">27.64</td>
<td align="char" char=".">60.12</td>
<td align="char" char=".">86.09</td>
<td align="char" char=".">12.52</td>
<td align="center">/</td>
<td align="char" char=".">1.39</td>
</tr>
<tr>
<td align="left">B03</td>
<td align="char" char=".">1.31</td>
<td align="char" char=".">0.83</td>
<td align="char" char=".">9.83</td>
<td align="char" char=".">26.60</td>
<td align="char" char=".">62.75</td>
<td align="char" char=".">92.34</td>
<td align="char" char=".">4.73</td>
<td align="center">0.37</td>
<td align="char" char=".">2.56</td>
</tr>
<tr>
<td align="left">D01</td>
<td align="char" char=".">1.56</td>
<td align="char" char=".">0.79</td>
<td align="char" char=".">11.54</td>
<td align="char" char=".">25.33</td>
<td align="char" char=".">62.35</td>
<td align="char" char=".">96.10</td>
<td align="char" char=".">1.60</td>
<td align="center">0.40</td>
<td align="char" char=".">1.90</td>
</tr>
<tr>
<td align="left">D02</td>
<td align="char" char=".">1.63</td>
<td align="char" char=".">0.93</td>
<td align="char" char=".">15.57</td>
<td align="char" char=".">21.57</td>
<td align="char" char=".">61.94</td>
<td align="char" char=".">96.30</td>
<td align="char" char=".">1.97</td>
<td align="center">/</td>
<td align="char" char=".">1.72</td>
</tr>
<tr>
<td align="left">D03</td>
<td align="char" char=".">1.93</td>
<td align="char" char=".">1.64</td>
<td align="char" char=".">9.27</td>
<td align="char" char=".">10.04</td>
<td align="char" char=".">79.05</td>
<td align="char" char=".">89.83</td>
<td align="char" char=".">9.22</td>
<td align="center">0.75</td>
<td align="char" char=".">0.19</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>
<italic>M</italic> is the moisture content, <italic>A</italic> is the ash content, <italic>V</italic> is the volatile matter content, and <italic>FC</italic> is the fixed carbon.</p>
</fn>
</table-wrap-foot>
</table-wrap>
<p>According to the different specific gravity values of each component, the vitrinite of the coal sample was separated and purified by hand picking and then density gradient centrifugation (<xref ref-type="bibr" rid="B11">Dyrkacz and Horwitz, 1982</xref>; <xref ref-type="bibr" rid="B16">Gilfillan et al., 1999</xref>; <xref ref-type="bibr" rid="B25">Ju et al., 2005b</xref>; <xref ref-type="bibr" rid="B51">Wang et al., 2005</xref>) to reduce the influence of coal components on the adsorption/desorption performance. Before the adsorption/desorption test, all deformed coal samples were crushed and sieved to 20&#x2013;40 mesh and then treated with vitrinite centrifugation based on hand-picked vitrinite. We used benzene and carbon tetrachloride (CCl<sub>4</sub>), which are volatile and have no effect on the coal structure, to refine the amount of vitrinite up to 80%&#x2013;99% (<xref ref-type="bibr" rid="B30">Li et al., 2010</xref>, <xref ref-type="bibr" rid="B31">2014</xref>). Please refer to previous articles for specific methods (<xref ref-type="bibr" rid="B11">Dyrkacz and Horwitz, 1982</xref>; <xref ref-type="bibr" rid="B25">Ju et al., 2005b</xref>; <xref ref-type="bibr" rid="B30">Li et al., 2010</xref>, <xref ref-type="bibr" rid="B31">2014</xref>).</p>
<p>Vitrinite accounts for between 81.90 and 96.30% of the samples, the inertinite content ranges from 1.60 to 12.52% and almost no liptinite is present. The mineral content ranges from 0.19 to 2.56%. As seen from <xref ref-type="table" rid="T2">Table 2</xref>, except for sample P01 (81.9%), the vitrinite content of all the other samples is above 85%, and the mineral content is below 3%. Therefore, these processes will increase the vitrinite content and minimize the effects of maceral composition on the pore structure.</p>
<sec id="s2-2-1">
<title>2.2.1 Scanning Electron Microscopy Observation</title>
<p>Scanning electron microscopy (SEM) can help us better understand the microstructure on small particle coal surfaces and analyze the fracture forms and internal structure of coal. SEM measurements were performed at Henan Polytechnic University. Coal samples collected were observed by SEM (JSM 6390/LV) with an acceleration voltage of 0.5&#x2013;30&#xa0;kV and 150&#x2013;3000&#xd7; magnification.</p>
</sec>
<sec id="s2-2-2">
<title>2.2.2 Adsorption Method</title>
<p>Before the adsorption experiments were performed, the eight samples were prepared by crushing and sieving the coal into three size ranges [0.12&#x2013;0.15&#xa0;mm (100&#x2013;120 mesh), 0.18&#x2013;0.25&#xa0;mm (60&#x2013;80 mesh), and 0.42&#x2013;0.84&#xa0;mm (20&#x2013;40 mesh)], followed by outgassing at 298&#xa0;K for 24&#xa0;h in a vacuum oven. This procedure was used to completely remove any adsorbed gas from the coal matrix. The coal samples were aerated with high-purity CH<sub>4</sub> (99.9%) and high-purity CO<sub>2</sub> (99.9%) under humidity/temperature balance conditions (0.93%/30&#xb0;C). Isothermal adsorption experiments were performed using an IS-300 automatic isothermal adsorption instrument. The pressure ranges used to measure gas adsorption were 0.5&#x2013;12&#xa0;MPa for CH<sub>4</sub> and 0.5&#x2013;5&#xa0;MPa for CO<sub>2</sub>. The adsorption capacity was determined at various pressures, and the adsorption equilibrium time was 24&#xa0;h.</p>
</sec>
<sec id="s2-2-3">
<title>2.2.3 Calculation of Langmuir Isotherms</title>
<p>Adsorb ability is a natural property of porous materials, including coal. The solid surface of coal and a gas form a system, and the phenomenon of gas components accumulating at the two-phase interface is called adsorption. The return of adsorbed gas molecules to the gas phase is called desorption. Coal adsorption is currently considered to involve mostly physical adsorption, as represented by the Langmuir adsorption model (<xref ref-type="bibr" rid="B29">Laxminarayana and Crosdale, 1999</xref>; <xref ref-type="bibr" rid="B55">Yu et al., 2004</xref>; <xref ref-type="bibr" rid="B39">Moore, 2012</xref>).</p>
<p>The Langmuir model is often referred to as monolayer adsorption theory, where the governing formula is simple and practical and has been widely used to describe gas adsorption in coal and other adsorbents. Most of the instruments used to measure isothermal adsorption in coal are designed in accordance with this theory. The Langmuir parametric formula is given as follows:<disp-formula id="e1">
<mml:math id="m1">
<mml:mrow>
<mml:mi>V</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>V</mml:mi>
<mml:mi mathvariant="normal">L</mml:mi>
</mml:msub>
<mml:mi>P</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mi mathvariant="normal">L</mml:mi>
</mml:msub>
<mml:mo>&#x2b;</mml:mo>
<mml:mi>P</mml:mi>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(1)</label>
</disp-formula>where <italic>P</italic> is the pressure of sorbate gas (MPa); <italic>V</italic> is the adsorption capacity under pressure P (m<sup>3</sup>/t); <italic>V</italic>
<sub>L</sub> is the Langmuir volume (m<sup>3</sup>/t); and <italic>P</italic>
<sub>L</sub> is the Langmuir pressure (MPa).</p>
<p>Defining A &#x3d; 1/<italic>V</italic>
<sub>L</sub> and B&#x3d;<italic>P</italic>
<sub>L</sub>/<italic>V</italic>
<sub>L</sub>, <xref ref-type="disp-formula" rid="e1">formula (1)</xref> can be written in terms of A, which is a function of <italic>P</italic>/<italic>V</italic> and <italic>P</italic>:<disp-formula id="e2">
<mml:math id="m2">
<mml:mrow>
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mo>/</mml:mo>
<mml:mi>V</mml:mi>
</mml:mrow>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mo>/</mml:mo>
<mml:mrow>
<mml:msub>
<mml:mi>V</mml:mi>
<mml:mi mathvariant="normal">L</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mrow>
<mml:mo>&#x2b;</mml:mo>
<mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mi mathvariant="normal">L</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mo>/</mml:mo>
<mml:msub>
<mml:mi>V</mml:mi>
<mml:mi mathvariant="normal">L</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mtext>&#x200a;</mml:mtext>
<mml:mi mathvariant="normal">o</mml:mi>
<mml:mi mathvariant="normal">r</mml:mi>
<mml:mtext>&#x200a;</mml:mtext>
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mo>/</mml:mo>
<mml:mi>V</mml:mi>
</mml:mrow>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>A</mml:mi>
<mml:mi>P</mml:mi>
<mml:mo>&#x2b;</mml:mo>
<mml:mi>B</mml:mi>
</mml:mrow>
</mml:math>
<label>(2)</label>
</disp-formula>
</p>
<p>
<xref ref-type="disp-formula" rid="e2">Formula (2)</xref> can be used to create scatter plots of the measured pressure and adsorption data at different equilibrium pressures with <italic>P</italic> as the abscissa and <italic>P/V</italic> as the ordinate. The regression formula and correlation coefficient of these scatter plots can be obtained by using the least squares method, where the slope of the straight line is <italic>A</italic> and the intercept is <italic>B</italic>. In this study, the slope and intercept were used to calculate the Langmuir volume and the Langmuir pressure as follows:<disp-formula id="e3">
<mml:math id="m3">
<mml:mrow>
<mml:msub>
<mml:mi>V</mml:mi>
<mml:mi mathvariant="normal">L</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>/</mml:mo>
<mml:mi>A</mml:mi>
</mml:mrow>
<mml:mo>,</mml:mo>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mi mathvariant="normal">L</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mi>B</mml:mi>
<mml:mo>/</mml:mo>
<mml:mi>A</mml:mi>
</mml:mrow>
<mml:mtext>&#x200a;</mml:mtext>
<mml:mi>o</mml:mi>
<mml:mi>r</mml:mi>
<mml:mtext>&#x200a;</mml:mtext>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mi mathvariant="normal">L</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:msub>
<mml:mi>V</mml:mi>
<mml:mi mathvariant="normal">L</mml:mi>
</mml:msub>
<mml:mi>B</mml:mi>
</mml:mrow>
</mml:math>
<label>(3)</label>
</disp-formula>
</p>
<p>The isothermal adsorption/desorption curve was plotted using the adsorption capacity and pressure for different equilibrium pressures.</p>
</sec>
</sec>
</sec>
<sec id="s3">
<title>3 Results</title>
<sec id="s3-1">
<title>3.1 Particle Characteristics of Coal From SEM Imaging</title>
<p>The grain fragments of undeformed coal, brittle deformed coal and ductile deformed coal were observed by SEM (<xref ref-type="fig" rid="F2">Figure 2</xref>). The undeformed coal (<xref ref-type="fig" rid="F2">Figures 2A&#x2013;D</xref>) grains are intact, the bedding is well preserved, and fractures are hardly observed. The pore distribution can be seen on the particle surface (red circle). In the brittle deformed coal (<xref ref-type="fig" rid="F2">Figures 2E&#x2013;J</xref>), fractures are developed, and particles are layered (<xref ref-type="fig" rid="F2">Figures 2E&#x2013;H</xref>). Smaller particles are sometimes observed agglomerating in fractures. Complete particles can be partially cut or fully penetrated by fractures, but the particles are still connected without further crushing. Due to fracture development, pores inside the particle are connected with surface pores (<xref ref-type="fig" rid="F2">Figures 2I,J</xref>). Wrinkles can also be seen on the particles of the ductile deformed coal, and flake particles can sometimes be observed (<xref ref-type="fig" rid="F2">Figures 2K&#x2013;P</xref>). Most of the ductile deformed coal particles are formed by agglomeration of small particles (<xref ref-type="fig" rid="F2">Figures 2K&#x2013;N</xref>), with a large number of pores, fractures and high connectivity, indicating that ductile deformation has caused the granulation of coal and destroyed its internal structure.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>SEM of images of <bold>(A&#x2013;D)</bold> undeformed coal, <bold>(E&#x2013;J)</bold> brittle deformed coal and <bold>(K&#x2013;P)</bold> ductile deformed coal.</p>
</caption>
<graphic xlink:href="feart-10-876196-g002.tif"/>
</fig>
</sec>
<sec id="s3-2">
<title>3.2 Adsorption Characteristics of Coal With Different Deformation Degrees</title>
<p>Adsorption data for the 8 samples were obtained from the abovementioned gas adsorption experiment, that is, adsorption of CH<sub>4</sub> and CO<sub>2</sub> for coal size fractions of 0.12&#x2013;0.15&#xa0;mm, 0.18&#x2013;0.25 and 0.42&#x2013;0.84&#xa0;mm. The results (on an air-dried basis) are presented in <xref ref-type="fig" rid="F3">Figure 3</xref>.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>CH<sub>4</sub> and CO<sub>2</sub> adsorption isotherms for coal samples with different size fractions.</p>
</caption>
<graphic xlink:href="feart-10-876196-g003.tif"/>
</fig>
<p>CH<sub>4</sub> adsorption: The CH<sub>4</sub> adsorption results are shown in the three left-hand-side images of <xref ref-type="fig" rid="F3">Figure 3</xref>, indicating that the adsorption capacity is lowest for undeformed coal and highest for high metamorphic grade and strong ductile deformed coal. The adsorption capacity of coal samples typically increases with the metamorphic grade (<xref ref-type="bibr" rid="B54">Yao and Liu, 2007</xref>; <xref ref-type="bibr" rid="B56">Zhang et al., 2009</xref>; <xref ref-type="bibr" rid="B2">Cai et al., 2013</xref>); however, <xref ref-type="fig" rid="F3">Figure 3</xref> shows that the adsorption capacity of P02 (<italic>R</italic>
<sub>o,max</sub> &#x3d; 1.29%) is always lower than that of P01 (<italic>R</italic>
<sub>o,max</sub> &#x3d; 0.97%) and two of the brittle deformed coals (B01 and B02). The adsorption capacity increases with the metamorphic grade when the samples are classified as brittle and ductile deformed coal. The adsorption isotherms of brittle deformed sample B03 (<italic>R</italic>
<sub>o,max</sub> &#x3d; 1.31%) and ductile deformed sample D03 (<italic>R</italic>
<sub>o,max</sub> &#x3d; 1.93%) lie above those of B01 and B02 (<italic>R</italic>
<sub>o,max</sub> &#x3d; 1.08 and 1.11%, respectively) and D01 and D02 (<italic>R</italic>
<sub>o,max</sub> &#x3d; 1.57 and 1.63%, respectively). In addition, the fixed carbon content values of the samples of brittle deformed coal B01&#x2013;03 and D01 are all between 60 and 62%, but their adsorption capacities vary greatly. The vitrinite content is lower in sample D03, which has the highest adsorption capacity (<xref ref-type="fig" rid="F3">Figure 3</xref> and <xref ref-type="table" rid="T2">Table 2</xref>). The influence of carbon and vitrinite on the gas adsorption capacity of coal is affected by structural deformation according to <xref ref-type="fig" rid="F3">Figure 3</xref> and <xref ref-type="table" rid="T2">Table 2</xref>. <xref ref-type="fig" rid="F3">Figure 3</xref> also shows that the adsorption capacities of the three brittle deformed coals (B01&#x2013;03) are larger than those of the high-rank weak ductile deformed coals (D01&#x2013;D02) but smaller than that of the high-rank strong ductile deformed coal (D03). Thus, the deformation degree also affects the adsorption capacity.</p>
<p>CO<sub>2</sub> adsorption: The three images on the right-hand side of <xref ref-type="fig" rid="F3">Figure 3</xref> show coal adsorption of CO<sub>2</sub>, which is known to be much greater than that of CH<sub>4</sub> (<xref ref-type="bibr" rid="B1">Busch et al., 2003</xref>; <xref ref-type="bibr" rid="B30">Li et al., 2010</xref>; <xref ref-type="bibr" rid="B18">Han et al., 2013</xref>; <xref ref-type="bibr" rid="B40">Mustafa et al., 2020</xref>). Undeformed coal has the lowest adsorption capacity, whereas high metamorphic grade and strong ductile deformed coal have the highest adsorption capacity; the same general trends are observed for the CH<sub>4</sub> adsorption isotherms, although the details are different. The low adsorption capacities of the two high-rank weak ductile deformed coals for the 0.18&#x2013;0.25&#xa0;mm size fraction, samples D01 (<italic>R</italic>
<sub>o,max</sub> &#x3d; 1.56%) and D02 (<italic>R</italic>
<sub>o,max</sub> &#x3d; 1.63%), are even lower than that of sample P01 (<italic>R</italic>
<sub>o,max</sub> &#x3d; 0.97%), which has the lowest rank of the 8 samples (<xref ref-type="fig" rid="F3">Figure 3</xref>). Thus, the adsorption capacity is also affected by the size fraction. Detailed results will be presented later.</p>
<p>The average Langmuir volumes for samples of the same type and size are plotted in <xref ref-type="fig" rid="F4">Figure 4</xref>. Irrespective of the particle size and coal type, the Langmuir volume for CO<sub>2</sub> adsorption is always larger than that for CH<sub>4</sub> adsorption. For the same coal type, the sample with a 0.18&#x2013;0.25&#xa0;mm particle size has a larger Langmuir volume than the other particle size samples (0.12&#x2013;0.15 and 0.42&#x2013;0.84&#xa0;mm). <xref ref-type="fig" rid="F4">Figure 4</xref> also shows that the ductile deformed coal has the largest Langmuir volume of all the coal samples.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>Langmuir volume of undeformed coal and deformed coal samples with different size fractions.</p>
</caption>
<graphic xlink:href="feart-10-876196-g004.tif"/>
</fig>
<p>The adsorption capacities decrease in the following order: strong ductile deformed coal &#x3e; brittle deformed coal &#x3e; weak ductile deformed coal &#x3e; undeformed coal. <xref ref-type="fig" rid="F3">Figure 3</xref> shows that the adsorption capacities of the three types of coal samples depend on the coal type, metamorphic grade, deformation process, adsorbed gas and size fraction.</p>
</sec>
<sec id="s3-3">
<title>3.3 Adsorption Characteristics of Coal With Different Particle Sizes</title>
<p>Undeformed coal (<xref ref-type="fig" rid="F5">Figure 5</xref>): For CH<sub>4</sub> adsorption, the sample with the largest particles (0.42&#x2013;0.84&#xa0;mm) has a smaller adsorption capacity than those with other particle sizes (0.18&#x2013;0.25 and 0.12&#x2013;0.15&#xa0;mm); that is, the adsorption capacities increase as the size fraction decreases. The coal samples with three particle sizes have similar CO<sub>2</sub> adsorption capacities in P01. The CO<sub>2</sub> adsorption isotherms of the 0.18&#x2013;0.25 and 0.42&#x2013;0.84&#xa0;mm samples are similar in P02 and smaller than that of the smallest particle (0.12&#x2013;0.15&#xa0;mm) sample.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Adsorption isotherms of undeformed coal samples, brittle and ductile deformed coal samples with different size fractions.</p>
</caption>
<graphic xlink:href="feart-10-876196-g005.tif"/>
</fig>
<p>Brittle deformed coal (<xref ref-type="fig" rid="F5">Figure 5</xref>): The CH<sub>4</sub> adsorption capacity of the 0.42&#x2013;0.84&#xa0;mm sample is always the smallest among the three particle size samples. The adsorption isotherms of the 0.18&#x2013;0.25&#xa0;mm coal sample are close for the 0.12&#x2013;0.15&#xa0;mm samples (B01 and B02), whereas that of B03 is slightly higher. The CO<sub>2</sub> adsorption isotherms for samples B01 and B03 with different size fractions of coal overlap; that is, there is little change in the adsorption capacity as the size fraction increases. However, the adsorption capacity slightly decreases as the size fraction decreases in sample B2.</p>
<p>Ductile deformed coal (<xref ref-type="fig" rid="F5">Figure 5</xref>): The CH<sub>4</sub> adsorption curves of samples of 0.42&#x2013;0.84&#xa0;mm are basically at the lowest level, which are greatly different from the adsorption curves of samples of 0.18&#x2013;0.25 and 0.12&#x2013;0.15&#xa0;mm. The adsorption curve of the 0.18&#x2013;0.25&#xa0;mm sample is basically greater than or similar to that of the 0.12&#x2013;0.15&#xa0;mm sample. The stronger the deformation is, the closer the adsorption curves of the two particle sizes are, indicating that the deformation increases the number of pores and adsorption sites of the samples to some extent, decreasing the influence of particle size on adsorption. The CO<sub>2</sub> adsorption isotherms of the three size fractions are similar, which means that the coal size fraction has little effect on the CO<sub>2</sub> adsorption capacity of brittle deformed coal.</p>
<p>
<xref ref-type="fig" rid="F5">Figure 5</xref> also show that the coal adsorption capacity is much higher for CO<sub>2</sub> than for CH<sub>4</sub> at the same pressure. The coal size fraction affects the adsorption capacity for CH<sub>4</sub> for all 8 samples; that is, the adsorption capacity increases as the size fraction decreases from 0.42&#x2013;0.84 to 0.18&#x2013;0.25&#xa0;mm. However, no obvious rule was found for the change in adsorption capacity from the 0.18&#x2013;0.25 to 0.12&#x2013;0.15&#xa0;mm samples. The coal size fraction has a slightly smaller influence on CO<sub>2</sub> adsorption than on CH<sub>4</sub> adsorption. Moreover, deformation appears to reduce the effect of particle size on the adsorption capacity, especially in ductile deformed coal.</p>
</sec>
<sec id="s3-4">
<title>3.4 Desorption Characteristics of Deformed Coal Samples With Different Particle Sizes</title>
<p>CH<sub>4</sub> and CO<sub>2</sub> desorption isotherms were routinely measured after conducting the adsorption experiments (<xref ref-type="fig" rid="F6">Figures 6</xref>, <xref ref-type="fig" rid="F7">7</xref>). All previous adsorption/desorption studies have shown that the desorption isotherm generally lies above the adsorption isotherm (<xref ref-type="bibr" rid="B18">Han et al., 2013</xref>; <xref ref-type="bibr" rid="B45">Romanov et al., 2013</xref>; <xref ref-type="bibr" rid="B46">Shi et al., 2020</xref>). This hysteresis effect indicates that the sorbent/sorbate system is in a metastable state and that decreasing the pressure does not readily release the gas to an extent corresponding to the thermodynamic equilibrium value (<xref ref-type="bibr" rid="B1">Busch et al., 2003</xref>). <xref ref-type="fig" rid="F6">Figures 6</xref>, <xref ref-type="fig" rid="F7">7</xref> show hysteresis curves of various shapes for CH<sub>4</sub> and CO<sub>2</sub> for the deformed sample set with different size fractions.</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>CH<sub>4</sub> adsorption/desorption isotherms of coal samples with different size fractions.</p>
</caption>
<graphic xlink:href="feart-10-876196-g006.tif"/>
</fig>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>CO<sub>2</sub> adsorption/desorption isotherms of coal samples with different size fractions.</p>
</caption>
<graphic xlink:href="feart-10-876196-g007.tif"/>
</fig>
<p>For CH<sub>4</sub> (<xref ref-type="fig" rid="F6">Figure 6</xref>), the 0.18&#x2013;0.25&#xa0;mm deformed coal samples exhibit the smallest deviations between the adsorption/desorption curves (little hysteresis), and all the samples release CH<sub>4</sub> in the first desorption step. However, the 0.42&#x2013;0.84&#xa0;mm deformed coal samples, with the exception of D03, exhibit strong hysteresis, and mass balance shows a slight increase in the excess sorption. Andreas et al. explained this effect in terms of small inaccuracies in the experimental values, but changes in the coal volume from compressibility or swelling are also a possible cause (<xref ref-type="bibr" rid="B1">Busch et al., 2003</xref>). Thus, small deformed coal particles can release CH<sub>4</sub> more easily than correspondingly larger particles. The desorption capacity of large coal particles increases under deformation.</p>
<p>For CO<sub>2</sub> (<xref ref-type="fig" rid="F7">Figure 7</xref>), the deformed coal samples of all size fractions exhibit similarly strong hysteresis, especially sample D01, whereas sample D03 exhibits the least hysteresis. There is a small increase in the excess sorption in the first desorption step for all the samples. No change is observed in the desorption isotherms of the two undeformed coal samples with different size fractions when metamorphism increases. The hysteresis of the brittle and ductile deformed coals decreases as the deformation increases; that is, deformation promotes CO<sub>2</sub> desorption. For the same size fraction, there is stronger hysteresis for CO<sub>2</sub> than CH<sub>4</sub>. The size fraction of the deformed coal samples clearly has no effect on the CO<sub>2</sub> desorption capacity, and CH<sub>4</sub> is more easily released than CO<sub>2</sub> in samples with the same size fraction. Furthermore, the higher desorption capacity of CH<sub>4</sub> relative to CO<sub>2</sub> decreases under deformation. That is, the effect of the size fraction on the gas desorption capacity of deformed coal is weakened by deformation.</p>
</sec>
<sec id="s3-5">
<title>3.5 Pore Size Distribution of Deformed Coal Samples With Different Particle Sizes</title>
<p>We compared the size distribution and parameters of coal pores for samples with different particle sizes, as obtained from a low-pressure CO<sub>2</sub> experiment. <xref ref-type="table" rid="T3">Table 3</xref> shows the pore structure parameters of coal with different size fractions, and <xref ref-type="fig" rid="F8">Figure 8</xref> show the pore size distribution (PSD) of undeformed coal and deformed coal with different size fractions.</p>
<table-wrap id="T3" position="float">
<label>TABLE 3</label>
<caption>
<p>Pore structure parameters obtained from CO<sub>2</sub> adsorption experiments on coal with different size fractions.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th rowspan="2" align="left"/>
<th colspan="3" align="center">0.42&#x2013;0.84 (mm)</th>
<th colspan="3" align="center">0.18&#x2013;0.25 (mm)</th>
<th colspan="3" align="center">0.12&#x2013;0.15 (mm)</th>
</tr>
<tr>
<th align="center">
<italic>V</italic> (cc/g)</th>
<th align="center">
<italic>S</italic> (m<sup>2</sup>/g)</th>
<th align="center">
<italic>w</italic> (nm)</th>
<th align="center">
<italic>V</italic> (cc/g)</th>
<th align="center">
<italic>S</italic> (m<sup>2</sup>/g)</th>
<th align="center">
<italic>w</italic> (nm)</th>
<th align="center">
<italic>V</italic> (cc/g)</th>
<th align="center">
<italic>S</italic> (m<sup>2</sup>/g)</th>
<th align="center">
<italic>w</italic> (nm)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">P01</td>
<td align="char" char=".">0.015</td>
<td align="char" char=".">36.89</td>
<td align="char" char=".">0.82</td>
<td align="char" char=".">0.019</td>
<td align="char" char=".">51.71</td>
<td align="char" char=".">0.55</td>
<td align="char" char=".">0.026</td>
<td align="char" char=".">78.74</td>
<td align="char" char=".">0.50</td>
</tr>
<tr>
<td align="left">P02</td>
<td align="char" char=".">0.017</td>
<td align="char" char=".">45.80</td>
<td align="char" char=".">0.82</td>
<td align="char" char=".">0.022</td>
<td align="char" char=".">60.25</td>
<td align="char" char=".">0.52</td>
<td align="char" char=".">0.034</td>
<td align="char" char=".">101.51</td>
<td align="char" char=".">0.50</td>
</tr>
<tr>
<td align="left">B01</td>
<td align="char" char=".">0.012</td>
<td align="char" char=".">32.44</td>
<td align="char" char=".">0.82</td>
<td align="char" char=".">0.028</td>
<td align="char" char=".">71.08</td>
<td align="char" char=".">0.80</td>
<td align="char" char=".">0.031</td>
<td align="char" char=".">92.60</td>
<td align="char" char=".">0.50</td>
</tr>
<tr>
<td align="left">B02</td>
<td align="char" char=".">0.023</td>
<td align="char" char=".">62.97</td>
<td align="char" char=".">0.8</td>
<td align="char" char=".">0.037</td>
<td align="char" char=".">99.71</td>
<td align="char" char=".">0.62</td>
<td align="char" char=".">0.040</td>
<td align="char" char=".">122.17</td>
<td align="char" char=".">0.50</td>
</tr>
<tr>
<td align="left">B03</td>
<td align="char" char=".">0.010</td>
<td align="char" char=".">26.76</td>
<td align="char" char=".">0.80</td>
<td align="char" char=".">0.028</td>
<td align="char" char=".">80.69</td>
<td align="char" char=".">0.52</td>
<td align="char" char=".">0.027</td>
<td align="char" char=".">76.75</td>
<td align="char" char=".">0.62</td>
</tr>
<tr>
<td align="left">D01</td>
<td align="char" char=".">0.011</td>
<td align="char" char=".">25.26</td>
<td align="char" char=".">0.82</td>
<td align="char" char=".">0.019</td>
<td align="char" char=".">51.35</td>
<td align="char" char=".">0.82</td>
<td align="char" char=".">0.018</td>
<td align="char" char=".">48.27</td>
<td align="char" char=".">0.52</td>
</tr>
<tr>
<td align="left">D02</td>
<td align="char" char=".">0.016</td>
<td align="char" char=".">41.10</td>
<td align="char" char=".">0.82</td>
<td align="char" char=".">0.220</td>
<td align="char" char=".">59.71</td>
<td align="char" char=".">0.52</td>
<td align="char" char=".">0.025</td>
<td align="char" char=".">73.26</td>
<td align="char" char=".">0.50</td>
</tr>
<tr>
<td align="left">D03</td>
<td align="char" char=".">0.051</td>
<td align="char" char=".">152.76</td>
<td align="char" char=".">0.50</td>
<td align="char" char=".">0.040</td>
<td align="char" char=".">130.4</td>
<td align="char" char=".">0.50</td>
<td align="char" char=".">0.060</td>
<td align="char" char=".">196.0</td>
<td align="char" char=".">0.48</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>PSD of undeformed and deformed coal with different size fractions.</p>
</caption>
<graphic xlink:href="feart-10-876196-g008.tif"/>
</fig>
<p>
<xref ref-type="fig" rid="F8">Figure 8</xref> shows the PSD of undeformed coal for three size fractions. As the particle size decreases, the pore diameter decreases, and the specific surface area of the pores increases. The PSD of deformed coal for three size fractions can be described as follows (<xref ref-type="fig" rid="F8">Figure 8</xref>): for weak brittle deformed coal (B1 and B2), as the particle size decreases, the pore specific surface area increases. However, in strong brittle deformed coal (B3), decreasing the particle size from 0.42&#x2013;0.84 to 0.18&#x2013;0.25&#xa0;mm reduces the pore size and increases the pore specific surface area. Further decreases in the particle size (from 0.18&#x2013;0.25 to 0.12&#x2013;0.15&#xa0;mm) do not affect the pores, and the pore specific surface area begins to decrease. In ductile deformed coal, similar changes are observed under weak deformation (D1 and D2) and strong brittle deformation. Under strong ductile deformation (D3), as the particle size decreases, the pore specific surface area increases.</p>
<p>The PSD characteristics showed good consistency with the adsorption capacity. When the adsorption gas is CH<sub>4</sub>, irrespective of the coal type, the largest sample size (0.42&#x2013;0.84&#xa0;mm) has the minimum pore specific surface area and adsorption/desorption volume (<xref ref-type="table" rid="T3">Table 3</xref>; <xref ref-type="fig" rid="F5">Figure 5</xref>). Opposite trends are observed for the adsorption/desorption volume and the specific surface area for the other particle sizes (0.18&#x2013;0.25 and 0.12&#x2013;0.15&#xa0;mm); that is, smaller particles lead to a smaller pore diameter and adsorption/desorption volume and a larger specific surface area. The smaller influence of the grain size on CO<sub>2</sub> adsorption than on CH<sub>4</sub> adsorption results from better penetration of the multisize pore structure of coal by CO<sub>2</sub> (<xref ref-type="bibr" rid="B37">Mastalerz et al., 2017</xref>), with CO<sub>2</sub> being smaller than CH<sub>4</sub> (kinetic diameters of CO<sub>2</sub> and CH<sub>4</sub> are 0.33 and 0.38 nm, respectively), and the influence of particle size on large pores is much stronger.</p>
</sec>
</sec>
<sec id="s4">
<title>4 Discussion</title>
<p>As the grain size of undeformed coal decreases, the abundance of 0.5&#x2013;0.6&#xa0;nm pores increase. However, a new pore size is added (&#x3c;0.5&#xa0;nm) when the grain size is 0.12&#x2013;0.15&#xa0;mm, and the pore sizes of other sizes are basically unchanged (<xref ref-type="fig" rid="F9">Figures 9</xref>, <xref ref-type="fig" rid="F10">10</xref>). Except for the D3 sample always having pores &#x3c;0.5 nm, the other deformed coal samples obviously have new pores (&#x3c;0.5&#xa0;nm and 1.0&#x2013;1.5&#xa0;nm pores) as grinding proceeds. Therefore, the smaller the particle size is, the larger the pore volume in deformed coal samples. Pores &#x3c;0.5&#xa0;nm are developed in D3 samples regardless of particle size, while pores &#x3c;0.5&#xa0;nm appear in other samples only when the particle size reaches 0.12&#x2013;0.15&#xa0;mm. <xref ref-type="fig" rid="F11">Figure 11</xref> shows the changes in pore structure with grain size and deformation degree. As the particle size of undeformed coal decreases, the abundance of pores larger than 30&#xa0;nm increases, and that of 2&#x2013;30&#xa0;nm pores decrease (<xref ref-type="bibr" rid="B21">Jia et al., 2013</xref>; <xref ref-type="bibr" rid="B37">Mastalerz et al., 2017</xref>). However, the content of pores of different sizes was reported to increase in deformed coal as the particle size decreased (<xref ref-type="bibr" rid="B12">Fan et al., 2013</xref>; <xref ref-type="bibr" rid="B31">Li, et al., 2014</xref>; <xref ref-type="bibr" rid="B52">Wang et al., 2021</xref>). Thus, strong structural deformation can replace grinding action to impart coal with smaller pores and more pore types with different pore sizes (<xref ref-type="fig" rid="F11">Figure 11</xref>).</p>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>Horizontal and stacked bar charts of undeformed coal and brittle deformed coal showing changes in the specific volume of micropore size ranges.</p>
</caption>
<graphic xlink:href="feart-10-876196-g009.tif"/>
</fig>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>Horizontal and stacked bar charts of ductile deformed coal showing changes in the specific volume of micropore size ranges.</p>
</caption>
<graphic xlink:href="feart-10-876196-g010.tif"/>
</fig>
<fig id="F11" position="float">
<label>FIGURE 11</label>
<caption>
<p>Schematic drawings of pore structure changes of coal with grain size and deformation degree (Part of data support from <xref ref-type="bibr" rid="B21">Jia et al., 2013</xref>; <xref ref-type="bibr" rid="B37">Mastalerz et al., 2017</xref>).</p>
</caption>
<graphic xlink:href="feart-10-876196-g011.tif"/>
</fig>
<p>If the sample collected includes deformed coal, the grain refinement caused by structural deformation must be considered in the sample preparation process. According to our experimental data, considering that the adsorption/desorption effects of the 0.12&#x2013;0.15 and 0.18&#x2013;0.25&#xa0;mm samples are similar, the particle size of 0.12&#x2013;0.15&#xa0;mm can ensure that all deformed coal samples have more diverse pore sizes and reduce the influence of structural deformation on particle size (<xref ref-type="fig" rid="F11">Figure 11</xref>). Therefore, if the adsorption/desorption characteristics of coal are studied from the perspective of structural deformation, it is recommended that the samples be crushed to 0.18&#x2013;0.25&#xa0;mm (60&#x2013;80 mesh) to achieve the ideal adsorption/desorption effect without eliminating the influence of structural deformation. If the influence of structural deformation is not taken into account but the sample contains deformed coal (due to the extensive development of deformed coal in China), it is recommended that the sample be crushed below 0.12&#x2013;0.15&#xa0;mm (100&#x2013;120 mesh) to reduce the impact of structural deformation on data processing and analysis (<xref ref-type="fig" rid="F11">Figure 11</xref>).</p>
<p>The results and discussion above show that coal with different deformations exhibits significantly different adsorption/desorption curves and pore structure characteristics for the same particle size. However, for the same deformation type, the adsorption/desorption curves and pore structure characteristics of samples with different particle sizes can be similar. Thus, deformation has a stronger influence on the adsorption/desorption performance and internal structure of coal than granularity. The stronger the deformation is, the smaller the impact of the particle size on the adsorption/desorption properties of coal. This result is obtained because deformation changes both the internal structure and the macromolecular structure of coal (<xref ref-type="bibr" rid="B44">Qu, 2011</xref>; <xref ref-type="bibr" rid="B33">Li et al., 2013</xref>, <xref ref-type="bibr" rid="B32">2017</xref>; <xref ref-type="bibr" rid="B27">Ju et al., 2018</xref>; <xref ref-type="bibr" rid="B53">Yang et al., 2020</xref>). Coal adsorption/desorption is closely related to coal pores, and the adsorption capacity is positively correlated with the total pore volume and the total pore specific surface area (<xref ref-type="bibr" rid="B54">Yao and Liu, 2007</xref>; <xref ref-type="bibr" rid="B20">Hou et al., 2017</xref>; <xref ref-type="bibr" rid="B37">Mastalerz et al., 2017</xref>; <xref ref-type="bibr" rid="B42">Pan et al., 2019</xref>). Structural deformation and sample granularity affect these parameters because the coal particle size is reduced by mechanical friction during deformation. The undeformed coal particles are intact, a few pores on the surface are connected to the outside, and the internal pores are still closed. However, the deformed coal particles are formed by agglomeration of smaller particles with more fractures distributed and more pores connected to the outside (<xref ref-type="fig" rid="F12">Figure 12</xref>). The pore volume and the specific surface area vary with the coal particle size, which changes the total number of adsorption sites. Studies have shown that structural deformation can decrease the number of side chain functional groups of coal macromolecular structures while increasing the content of benzene ring structures and aromatic lamellar structures. Both the benzene ring structure and the lamellar gap can increase the gas adsorption/desorption potential and the gas adsorption capacity (<xref ref-type="bibr" rid="B5">Cao et al., 2003b</xref>; <xref ref-type="bibr" rid="B26">Ju and Li, 2009</xref>; <xref ref-type="bibr" rid="B58">Zhou 2010</xref>; <xref ref-type="bibr" rid="B31">Li et al., 2014</xref>; <xref ref-type="bibr" rid="B53">Yang et al., 2020</xref>). Therefore, structural deformation can also change the adsorption/desorption properties of coal <italic>via</italic> the macromolecular structure, which does not only depend on simple granularity factors.</p>
<fig id="F12" position="float">
<label>FIGURE 12</label>
<caption>
<p>Schematic diagram of characteristics of undeformed and deformed coal particles.</p>
</caption>
<graphic xlink:href="feart-10-876196-g012.tif"/>
</fig>
</sec>
<sec id="s5">
<title>5 Conclusion</title>
<p>
<list list-type="simple">
<list-item>
<p>1) Structural deformation has a great effect on the coal particles and internal structure, causes the granulation of coal and destroys its internal structure. The deformed coal particles and internal structure are formed by agglomeration of smaller particles with more fractures distributed and more pores connected to the outside. This means that deformed coal can provide more adsorption sites and adsorption space.</p>
</list-item>
<list-item>
<p>2) The adsorption capacity is always larger and faster for CO<sub>2</sub> than for CH<sub>4</sub> under the same pressure in deformed and undeformed coal. The adsorption capacities for CH<sub>4</sub> and CO<sub>2</sub> decrease in the following order: strong ductile deformed coal &#x3e; brittle deformed coal &#x3e; weak ductile deformed coal &#x3e; undeformed coal.</p>
</list-item>
<list-item>
<p>3) A larger influence of the grain size and internal structure is observed on the adsorption/desorption of CH<sub>4</sub> than that of CO<sub>2</sub>. Deformation affects the adsorption/desorption performance and the coal pore structure more strongly than granularity. The stronger the deformation is, the smaller the effect of the particle size and internal structure on coal adsorption/desorption. This relationship indicates that strong structural deformation can replace grinding action to impart coal with smaller pores and more pore types with different pore sizes.</p>
</list-item>
<list-item>
<p>4) The optimal size and internal structure during the adsorption experiment of deformed coal has been established, which can produce good-quality adsorption data of deformed coal for comparison with results from different studies. Our results demonstrate that the 0.18&#x2013;0.25&#xa0;mm (60&#x2013;80 mesh) fraction for coal appears to be optimal and the most practical size range and internal structure for performing adsorption analysis if it is necessary to consider the influence of structural deformation. If the influence of structural deformation is not considered but the sample contains deformed coal (due to the extensive development of deformed coal in China), it is recommended that the sample be crushed below a smaller granularity (0.12&#x2013;0.15&#xa0;mm) to reduce the impact of structural deformation on data processing and analysis.</p>
</list-item>
</list>
</p>
</sec>
</body>
<back>
<sec id="s6">
<title>Data Availability Statement</title>
<p>The original contributions presented in the study are included in the article/supplementary files, further inquiries can be directed to the corresponding author.</p>
</sec>
<sec id="s7">
<title>Author Contributions</title>
<p>XL: Conceptualization, Data curation, Formal analysis, Writing- Original draft preparation. Visualization, Writing&#x2014;review and editing. YJ: Writing&#x2014;review and editing, Funding acquisition, Project administration. YS: Writing&#x2014;review and editing. ZY: Resources, Investigation. QL: Resources, Investigation.</p>
</sec>
<sec id="s8">
<title>Funding</title>
<p>This work was supported by the National Natural Science Foundation of China (Grant Nos. 41672201, 41530315, 40972131, 41202120).</p>
</sec>
<sec sec-type="COI-statement" id="s9">
<title>Conflict of Interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec sec-type="disclaimer" id="s10">
<title>Publisher&#x2019;s Note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
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